Preface to the Second Edition |
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xv | |
Preface to the First Edition |
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xvii | |
Part I From Maxwell's Equations To Magnetohydrodynamics |
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1 | (120) |
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1 A Qualitative Overview of MHD |
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3 | (24) |
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3 | (3) |
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1.2 A Brief History of MHD |
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6 | (1) |
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1.3 From Electrodynamics to MHD: A Simple Experiment |
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7 | (10) |
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1.3.1 Some Important Parameters in Electrodynamics and MHD |
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8 | (1) |
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1.3.2 Electromagnetism Remembered |
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8 | (3) |
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1.3.3 A Familiar High School Experiment |
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11 | (6) |
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1.4 A Glimpse at the Astrophysical and Terrestrial Applications of MHD |
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17 | (7) |
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24 | (3) |
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2 The Governing Equations of Electrodynamics |
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27 | (30) |
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2.1 The Electric Field and the Lorentz Force |
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27 | (2) |
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2.2 Ohm's Law and the Volumetric Lorentz Force |
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29 | (2) |
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2.3 Ampere's Law and the Biot-Savart Law |
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31 | (3) |
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2.4 Faraday's Law and the Vector Potential |
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34 | (3) |
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2.5 An Historical Aside: Faraday and the Concept of the Field |
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37 | (3) |
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40 | (7) |
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2.6.1 The Displacement Current and Electromagnetic Waves |
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41 | (2) |
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2.6.2 Gauges, Retarded Potentials and the Biot-Savart Law Revisited |
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43 | (4) |
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2.7 The Reduced Form of Maxwell's Equations for MHD |
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47 | (2) |
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2.8 A Transport Equation for the Magnetic Field |
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49 | (1) |
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2.9 A Second Look at Faraday's Law |
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49 | (7) |
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2.9.1 An Important Kinematic Equation |
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50 | (1) |
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2.9.2 The Full Significance of Faraday's Law |
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51 | (2) |
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2.9.3 Faraday's Law in Ideal Conductors: Alfven's Theorem |
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53 | (3) |
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56 | (1) |
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3 A First Course in Fluid Dynamics |
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57 | (55) |
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3.1 Different Categories of Fluid Flow |
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57 | (12) |
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3.1.1 Viscosity, the Reynolds Number and Boundary Layers |
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58 | (4) |
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3.1.2 Laminar Versus Turbulent Flow |
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62 | (3) |
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3.1.3 Rotational Versus Irrotational flow |
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65 | (4) |
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3.2 The Navier-Stokes Equation |
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69 | (1) |
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3.3 Vorticity, Angular Momentum, and the Biot-Savart Law |
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70 | (4) |
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3.4 The Vorticity Equation and Vortex Line Stretching |
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74 | (6) |
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80 | (5) |
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80 | (1) |
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81 | (2) |
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3.5.3 Helicity Conservation |
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83 | (2) |
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85 | (6) |
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3.6.1 The Dissipation of Energy |
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85 | (1) |
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86 | (2) |
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3.6.3 The Prandtl-Batchelor Theorem |
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88 | (3) |
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3.7 Boundary Layers, Reynolds Stresses and Elementary Turbulence Models |
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91 | (7) |
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91 | (2) |
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3.7.2 Turbulence and Simple Turbulence Models |
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93 | (5) |
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3.8 Ekman Layers and Ekman Pumping in Rotating Fluids |
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98 | (3) |
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3.9 Waves and Columnar Vortices in Rotating Fluids |
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101 | (9) |
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3.9.1 The Taylor-Proudman Theorem |
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102 | (1) |
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3.9.2 Inertial Waves, Helicity Transport and the Formation of Taylor Columns |
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103 | (3) |
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3.9.3 Inertial Wave Packets, Columnar Vortices and Transient Taylor Columns |
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106 | (3) |
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3.9.4 A Glimpse at Rapidly Rotating Turbulence |
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109 | (1) |
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110 | (2) |
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4 The Governing Equations of MHD |
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112 | (9) |
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4.1 The MHD Equations and Key Dimensionless Groups |
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112 | (4) |
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4.2 Energy Considerations |
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116 | (1) |
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4.3 Maxwell's Stresses and Faraday's Tension |
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117 | (3) |
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4.4 A Glimpse at Alfven Waves |
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120 | (1) |
Part II The Fundamentals Of Incompressible MHD |
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121 | (184) |
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5 Kinematics: Advection, Diffusion and Intensification of Magnetic Fields |
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123 | (21) |
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5.1 The Analogy to Vorticity |
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123 | (1) |
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5.2 Diffusion of a Magnetic Field |
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124 | (1) |
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5.3 Advection in Ideal Conductors: Alfven's Theorem |
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125 | (3) |
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125 | (1) |
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126 | (2) |
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5.4 Helicity Invariants in Ideal MHD |
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128 | (3) |
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128 | (2) |
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5.4.2 Minimum Energy states |
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130 | (1) |
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131 | (1) |
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5.5 Advection Plus Diffusion |
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131 | (10) |
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132 | (1) |
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133 | (3) |
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5.5.3 Azimuthal Field Generation by Differential Rotation: The Ω-Effect |
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136 | (1) |
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5.5.4 Stretched Flux Tubes and Current Sheets |
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137 | (2) |
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5.5.5 Magnetic Reconnection |
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139 | (2) |
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5.6 Field Generation by Flux-Tube Stretching: A Glimpse at Dynamo Theory |
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141 | (1) |
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142 | (2) |
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6 Dynamics at Low Magnetic Reynolds Numbers |
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144 | (41) |
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6.1 The Low Magnetic Reynolds Number Approximation |
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145 | (1) |
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6.2 The Suppression of Motion |
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146 | (19) |
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146 | (2) |
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6.2.2 The Damping of a Two-Dimensional Jet |
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148 | (1) |
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6.2.3 The Damping of a Vortex |
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149 | (6) |
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6.2.4 The Damping of Turbulence at Low Rm |
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155 | (4) |
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6.2.5 Natural Convection in a Magnetic Field: Rayleigh-Benard Convection |
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159 | (6) |
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6.3 An Aside: A Glimpse at the Damping of Turbulence at Arbitrary Rm |
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165 | (3) |
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6.4 The Generation of Motion |
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168 | (10) |
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6.4.1 Rotating Fields and Swirling Motion |
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168 | (3) |
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6.4.2 Swirling Flow Induced between Two Parallel Plates |
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171 | (3) |
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6.4.3 Flows Resulting from Current Injection |
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174 | (4) |
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6.5 Boundary Layers and Associated Duct Flows |
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178 | (5) |
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6.5.1 Hartmann Boundary Layers |
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178 | (3) |
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6.5.2 Pumps, Propulsion and Projectiles |
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181 | (2) |
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183 | (2) |
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7 Dynamics at High Magnetic Reynolds Numbers |
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185 | (43) |
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7.1 Alfven Waves and Elsasser Variables |
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187 | (3) |
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7.2 Finite-Amplitude Alfven Waves and the Conservation of Cross Helicity |
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190 | (2) |
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7.3 Colliding Alfven Wave Packets and a Glimpse at Alfvenic Turbulence |
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192 | (3) |
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7.4 Magnetostrophic Waves |
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195 | (2) |
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7.5 The Energy Principle for Magnetostatic Equilibria in Ideal Fluids |
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197 | (12) |
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7.5.1 The Need for Stability in Plasma Confinement |
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198 | (3) |
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7.5.2 The Stability of Static Equilibria: A Variational Approach |
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201 | (5) |
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7.5.3 The Stability of Static Equilibria: A Direct Attack |
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206 | (3) |
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7.6 An Energy-Based Stability Theorem for Non-Static Equilibria |
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209 | (6) |
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7.7 The Chandrasekhar-Velikhov Instability in Rotating MHD |
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215 | (9) |
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7.7.1 The Magnetic Destabilisation of Rotating Flow |
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216 | (4) |
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7.7.2 The Energy Principle Applied to Rotating MHD |
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220 | (2) |
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7.7.3 The Destabilising Influence of an Azimuthal Field |
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222 | (1) |
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7.7.4 The Destabilising Influence of an Axial Field |
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223 | (1) |
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7.8 From MHD to Euler Flows: The Kelvin-Arnold Theorem |
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224 | (2) |
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226 | (2) |
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8 An Introduction to Turbulence |
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228 | (49) |
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8.1 An Historical Interlude |
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229 | (4) |
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8.2 The Structure of Turbulent Flows: Richardson's Cascade |
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233 | (6) |
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8.3 Kinematic Preliminaries (for Homogeneous Turbulence) |
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239 | (16) |
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8.3.1 Correlation Functions and Structure Functions |
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239 | (5) |
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244 | (5) |
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8.3.3 The Special Case of Statistically Isotropic Turbulence |
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249 | (6) |
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8.4 Kolmogorov's Theory of the Small Scales |
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255 | (4) |
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8.5 The Karman-Howarth Equation |
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259 | (7) |
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8.5.1 The Karman-Howarth Equation and the Closure Problem |
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259 | (3) |
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8.5.2 The Four-Fifths Law |
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262 | (2) |
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264 | (2) |
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8.6 Freely Decaying Turbulence |
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266 | (11) |
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8.6.1 Saffman versus Batchelor Turbulence: Two Canonical Energy Decays Laws |
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266 | (5) |
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8.6.2 Long-Range Interactions in Turbulence |
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271 | (2) |
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8.6.3 Landau's Theory: The Role of Angular Momentum Conservation |
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273 | (2) |
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8.6.4 Problems with Landau's Theory and Its Partial Resolution |
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275 | (2) |
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9 MHD Turbulence at Low and High Magnetic Reynolds Numbers |
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277 | (28) |
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9.1 The Growth of Anisotropy at Low and High Rm |
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277 | (4) |
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9.2 Loitsyansky and Saffman-like Invariants for MHD Turbulence at Low Rm |
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281 | (5) |
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9.3 Decay Laws for Fully Developed MHD Turbulence at Low Rm |
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286 | (2) |
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9.4 The Spontaneous Growth of a Seed Field at High Rm: Batchelor's Criterion |
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288 | (3) |
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9.5 Magnetic Field Generation in Forced, Non-Helical Turbulence at High Rm |
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291 | (6) |
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9.5.1 Different Categories of Magnetic Field Generation |
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292 | (2) |
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9.5.2 A Kinematic Model for Field Generation in Forced, Non-Helical Turbulence |
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294 | (2) |
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9.5.3 The Role of the Magnetic Reynolds and Magnetic Prandtl Numbers |
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296 | (1) |
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9.6 Unforced, Helical Turbulence at High Magnetic Reynolds Numbers |
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297 | (10) |
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9.6.1 Ideal Invariants and Selective Decay |
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298 | (2) |
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300 | (1) |
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9.6.3 Dynamic Alignment and Alfvenic States |
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301 | (4) |
Part III Applications In Engineering And Materials |
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305 | (94) |
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10 The World of Metallurgical MHD |
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307 | (10) |
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10.1 The History of Electrometallurgy |
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307 | (3) |
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10.2 An Overview of the Role of Magnetic Fields in Materials Processing |
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310 | (7) |
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11 The Generation and Suppression of Motion in Castings |
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317 | (34) |
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11.1 Magnetic Stirring Using Rotating Fields |
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317 | (15) |
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11.1.1 Casting, Stirring and Metallurgy |
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317 | (3) |
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11.1.2 The Magnetic Teaspoon |
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320 | (2) |
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11.1.3 Simple Models of Stirring |
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322 | (3) |
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11.1.4 The Role of Secondary Flows in Steel Casting |
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325 | (2) |
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11.1.5 The Role of Ekman Pumping for Non-Ferrous Metals |
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327 | (5) |
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11.2 Magnetic Damping Using Static Fields |
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332 | (19) |
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11.2.1 Metallurgical Applications |
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332 | (2) |
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11.2.2 The Need to Conserve Momentum in the Face of Joule Dissipation |
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334 | (3) |
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11.2.3 The Magnetic Damping of Submerged Jets |
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337 | (5) |
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11.2.4 The Magnetic Damping of Vortices |
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342 | (9) |
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12 Axisymmetric Flows Driven by the Injection of Current |
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351 | (23) |
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12.1 The Need to Purify Metal for Critical Aircraft Parts: Vacuum-Arc Remelting |
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351 | (3) |
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354 | (2) |
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12.3 Integral Constraints and the Work Done by the Lorentz Force |
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356 | (3) |
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12.4 Structure and Scaling of the Flow |
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359 | (5) |
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12.4.1 Confined versus Unconfined Domains |
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359 | (2) |
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12.4.2 Shercliff's Solution for Unconfined Domains |
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361 | (2) |
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363 | (1) |
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12.5 The Influence of Buoyancy |
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364 | (2) |
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12.6 The Apparent Spontaneous Growth of Swirl |
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366 | (3) |
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12.6.1 An Extraordinary Experiment |
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366 | (2) |
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12.6.2 But There Is no Spontaneous Growth of Swirl! |
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368 | (1) |
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12.6.3 Flaws in Traditional Theories Predicting a Spontaneous Growth of Swirl |
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369 | (1) |
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12.7 Poloidal Suppression versus Spontaneous Swirl |
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369 | (5) |
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13 MHD Instabilities in Aluminium Reduction Cells |
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374 | (25) |
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13.1 The Prohibitive Cost of Reducing Alumina to Aluminium |
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374 | (3) |
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13.1.1 Early Attempts to Produce Aluminium by Electrolysis |
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374 | (2) |
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13.1.2 An Instability in Modern Reduction Cells and Its Financial consequences |
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376 | (1) |
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13.2 Attempts to Model Unstable Interfacial Waves in Reduction Cells |
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377 | (2) |
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13.3 A Simple Mechanical Analogue for the Instability |
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379 | (5) |
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13.4 Simplifying Assumptions and a Model Problem |
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384 | (2) |
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13.5 A Shallow-Water Wave Equation for the Model Problem |
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386 | (4) |
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13.5.1 The Shallow-Water Wave Equations |
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386 | (3) |
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13.5.2 Key Dimensionless Groups |
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389 | (1) |
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13.6 Solutions of the Wave Equation |
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390 | (7) |
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390 | (1) |
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13.6.2 Standing Waves in Circular Domains |
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391 | (1) |
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13.6.3 Standing Waves in Rectangular Domains |
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392 | (5) |
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13.7 Implications for Cell Design and Potential Routes to Saving Energy |
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397 | (1) |
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398 | (1) |
Part IV Applications In Physics |
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399 | (142) |
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401 | (81) |
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14.1 Why Do We Need a Dynamo Theory for the Earth? |
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401 | (3) |
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14.2 Sources of Convection, Reversals and Key Dimensionless Groups |
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404 | (6) |
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14.2.1 The Structure of the Earth and Sources of Convection |
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404 | (1) |
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14.2.2 Field Structure and Reversals |
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405 | (3) |
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14.2.3 Key Dimensionless Groups |
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408 | (2) |
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14.3 A Comparison with the Other Planets |
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410 | (6) |
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14.3.1 The Properties of the Other Planets |
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410 | (3) |
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14.3.2 Trends in the Strengths of the Planetary Dipoles: Scaling Laws |
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413 | (3) |
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14.4 Tentative Constraints on Planetary Dynamo Theories |
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416 | (2) |
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14.5 Elementary Kinematic Theory: Phenomena, Theorems and Dynamo Types |
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418 | (22) |
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14.5.1 A Survey: Six Important Kinematic Results |
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418 | (3) |
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14.5.2 A Large Magnetic Reynolds Number Is Required |
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421 | (1) |
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14.5.3 Differential Rotation in the Core and the Omega-Effect |
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422 | (5) |
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14.5.4 An Axisymmetric Dynamo Is not Possible: Cowling's Theorem |
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427 | (2) |
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14.5.5 An Evolution Equation for the Axial Field |
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429 | (2) |
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14.5.6 A Glimpse at Parker's Helical Dynamo Mechanism |
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431 | (5) |
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14.5.7 Different Classes of Planetary Dynamo |
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436 | (4) |
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14.6 Building on Parker's Helical Lift-and-Twist Mechanism |
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440 | (10) |
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14.6.1 Mean-Field Electrodynamics |
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440 | (2) |
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14.6.2 A More Careful Look at the a-Effect |
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442 | (4) |
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14.6.3 Exact Integrals Relating the Large-Scale Field to the Small-Scale EMF |
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446 | (2) |
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14.6.4 Putting the Pieces Together: A Kinematic Criterion for Dynamo Action |
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448 | (2) |
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14.7 The Numerical Simulations of Planetary Dynamos |
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450 | (3) |
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14.8 Speculative Dynamo Cartoons Based on the Numerical Simulations |
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453 | (9) |
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14.8.1 Searching for the Source of the North-South Asymmetry in Helicity |
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453 | (3) |
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14.8.2 A Speculative Weak-Field Cartoon |
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456 | (5) |
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14.8.3 A Speculative Strong-Field Cartoon |
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461 | (1) |
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14.9 Dynamics of the Large Scale: the Taylor Constraint |
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462 | (2) |
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14.10 Laboratory Dynamo Experiments |
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464 | (5) |
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14.10.1 Two Classic Experiments |
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465 | (2) |
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14.10.2 More Recent Experiments |
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467 | (2) |
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14.11 Scaling Laws for Planetary Dynamos (Reprise) |
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469 | (3) |
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472 | (10) |
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482 | (32) |
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483 | (13) |
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15.1.1 The Sun's Interior and Atmosphere |
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483 | (3) |
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15.1.2 Is There a Solar Dynamo? |
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486 | (1) |
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15.1.3 Sunspots and the 11-Year Solar Cycle |
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487 | (1) |
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15.1.4 The Location of the Solar Dynamo and Dynamo Cartoons |
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488 | (4) |
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15.1.5 Prominences, Flares and Coronal Mass ejections |
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492 | (4) |
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496 | (5) |
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15.2.1 Why Is There a Solar Wind? |
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496 | (2) |
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15.2.2 Parker's Model of the Solar Wind |
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498 | (3) |
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501 | (13) |
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15.3.1 The Basic Properties of Accretion Discs |
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502 | (5) |
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15.3.2 The Standard Model of Accretion Discs |
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507 | (5) |
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15.3.3 The Chandrasekhar-Velikhov Instability Revisited |
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512 | (2) |
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16 Plasma Containment in Fusion Reactors |
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514 | (27) |
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16.1 The Quest for Controlled Fusion Power |
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514 | (1) |
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16.2 The Requirements for Controlled Nuclear Fusion |
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515 | (2) |
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16.3 Magnetic Confinement and the Instability of Fusion Plasmas |
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517 | (15) |
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16.3.1 The Topology of Confinement |
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517 | (1) |
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16.3.2 Sausage-Mode and Kink Instabilities Revisited |
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518 | (6) |
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16.3.3 Axisymmetric Internal Modes |
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524 | (2) |
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16.3.4 Interchange and Ballooning Modes |
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526 | (6) |
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16.4 The Development of Tokamak Reactors |
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532 | (4) |
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16.5 Tritium Breeding and Heat Extraction: MHD Channel Flow Revisited |
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536 | (3) |
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539 | |
Appendices |
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Appendix A Vector Identities and Theorems |
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541 | (2) |
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Appendix B Physical Properties of Liquid Metals |
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543 | (1) |
References |
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544 | (7) |
Index |
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551 | |